Diffractive DIS dijet cross section measured differentially as a function of $\log x_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively. (Note: assume typo in Table 2 that $x_P$ really means $\log x_P$.).

Diffractive DIS dijet cross section measured differentially as a function of $z_P$. The global normalisation uncertainty of $7.8\%$ is not listed explicitly but is included in the total systematic uncertainty. The last two column show the correction factors for hadronisation and QED radiation, respectively.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,1}$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{T,2}$.

Diffractive DIS dijet cross section measured differentially as a function of $\langle p^{\ast}_{T}\rangle$.

Diffractive DIS dijet cross section measured differentially as a function of $\Delta\eta^{\ast}$.

Diffractive DIS dijet cross section measured differentially as a function of $z_P$ and $Q^2$.

Diffractive DIS dijet cross section measured differentially as a function of $p^{\ast}_{\rm T,1}$ and $Q^2$.

Bin averaged hadron level differential cross sections as a function of the variable $z_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $x_{I\!\!P}$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $y$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections as a function of the variable $Q^2$ for diffractive dijet DIS. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential cross sections for diffractive dijet DIS as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations and the the radiative corrections ($1+\delta_{\text{rad}}$) are also listed. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $z_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_{I\!\!P}$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $y$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections as a function of the variable $x_\gamma$ for the dijet photoproduction kinematic range. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $M_X$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Bin averaged hadron level differential diffractive dijet $ep$ cross sections in the photoproduction kinematic range as a function of the variable $\langle\eta^{\text{jets}}\rangle$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given. The overall normalisation uncertainty of $6\%$ is not included in the table.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $\vert\Delta\eta^{\text{jets}}\vert$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $y$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $z_{I\!\!P}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

Ratios of differential diffractive dijet $ep$ cross sections, measured in photoproduction, to measurements in DIS as a function of the variable $E_T^{*\text{jet1}}$. The hadronisation correction factors ($1+\delta_{\text{hadr}}$) applied to the NLO calculations are given.

The differential cross section as a function of pseudorapidity.

The differential cross section as a function of log(M(P=5)**2).

The differential cross section as a function of X(C=D*).

The differential cross section as a function of BETA.

The differential cross section as a function of LOG(BETA).

The differential cross section as a function of LOG(Q**2).

The differential cross section as a function of W.

Overall ratio of diffractively produced D*+- mesons to inclusive D*+- mesons.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of transverse momentum.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of pseudorapidity.

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of X(C=D*).

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of LOG(Q**2).

Ratio of diffractively produced D*+- mesons to inclusive D*+- mesons as a function of W.

Differential cross section as a function of LOG(BETA) in different regions of Q**2 and X(NAME=POMERON).

The measured charm contribution to the diffractive structure function of the proton F2(C=D(3),CHARM).

Differential cross section w.r.t. Q**2.

Differential cross section w.r.t. W.

Differential cross section w.r.t. X(C=POMERON).

Differential cross section w.r.t. BETA.

Differential cross section w.r.t. PT(D*+-).

Differential cross section w.r.t. ETARAP.

The two-photon cross section as a function of the photon virtualities Qi**2. H ere Q1 is the virtuality w.r.t the electron vertex, and Q2 w.r.t the positron vertex. Data are given both before and after radiative corrections.

The two-photon cross section as a function of W, the invariant mas of the vir tual GAMMA*GAMMA* system. Data are given both before and after radiative corrections.

The two-photon cross section as a function of LN(W**2/Q1*Q2). Data are given both before and after radiative corrections.

Differential cross section as a function of the ratio of the virtualities of the two photons.

Differential cross section as a function of the acolinearity angle PHI between the scattered electrons.

Differential cross section as a function of the acolinearity angle DEL(PHI) between the scattered electrons.

Differential cross section as a function of W of the hadronic system.

Differential cross section as a function of the Bjorken X.

Differential cross section as a function of the DIS Y variable.

Differential cross section as a function of LOG(S/S0).

Cross section as a function of Z(NAME=POMERON,C=OBSERVED).

Cross section as a function of LOG10(Q**2).

Cross section as a function of PT(P=4,RF=CM).

Cross section as a function of ETARAP(P=4).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of the invariant mass of the diffractive system (X).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of W.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of X(NAME=POMERON).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of BETA=X/X(NAME=POMERON).

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), the fraction of the hadronic final state energy of the DD system which is contained in the two jets.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of X(NAME=GAMMA,C=JETS), the fraction ofthe photon momentum which enters the hard scattering.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of E(NAME=REM,C=GAMMA), the energy sum of all final state hadrons in the photon hemisphere (ETARAP<0) which lie outside the two hightest PT(RF=CM) jet cones.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -1.5 TO -1.3.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -1.75 TO -1.5.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range -2.0 TO -1.75.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the LOG10(X(NAME=POMERON)) range < -2.0.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 20 TO 35 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 35 TO 45 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range 45 TO 60 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), for the Q**2 + PT**2 range > 60 GEV**2.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Q**2 for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of the average transverse momentum of the two jets in the c.m.frame for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of Z(NAME=POMERON,C=JETS), the fraction of the hadronic final state energy of the DD system which is contained in the two jets for the restricted interval X(NAME=POMERON) < 0.01.

Average values, over the specified interval, of the differential hadron level dijet cross section as a function of PT(NAME=REM,C=POMERON), the PT sum of all final state hadrons in the pomeron hemisphere (ETARAP>0) which lie outside the two hightest PT(RF=CM) jet cones.

Average values, over the specified interval, of the differential hadron level three-jet cross section as a function of the invariant mass of the 3 jet system.

Average values, over the specified interval, of the differential hadron level three-jet cross section as a function of Z(NAME=POMERON,C=3-JETS).

Differential cross section as a function of W.

Differential cross section as a function of DELTA(PHI), where DELTA(PHI) is the angle between the azimuthal angles of the two virtual photons.

Differential cross section as a function of YBAR, where YBAR is defined as LN(W**2/SQRT(Q1**2 * Q2**2)).

Cross section as a function of X where X is the maximum value of X1 or X2, the upper and lower vertex values.

Cross section as a function of Q**2 where Q**2 is the maximum value of Q1**2 or Q2**2, the upper and lower vertex values.

Cross section as a function of W.

Cross section as a function of DELTA(PHI), where DELTA(PHI) is the angle between the azimuthal angles of the two virtual photons.

Cross section as a function of YBAR, where YBAR is defined as LN(W**2/SQRT(Q1**2 * Q2**2)).